$A$ conducting square loop of side $L$ and resistance $R$ moves in its plane with a uniform velocity $v$ perpendicular to one of its sides. $A$ magnetic induction $B$ constant in time and space,pointing perpendicular and into the plane of the loop exists everywhere. The current induced in the loop is

  • A
    $\frac{BLv}{R}$ clockwise
  • B
    $\frac{BLv}{R}$ anticlockwise
  • C
    $\frac{2BLv}{R}$ anticlockwise
  • D
    Zero

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